交流异步电机的Modelica模型

Modelica标准库里的异步电机模型过于复杂，为了便于学习，我用最基本的异步电机方程写了一个Modelica模型，公式参照陈伯时的《电力拖动自动控制系统--运动控制系统》第3版的190页到195页的内容，实际的电机模型参数参照了Novotny和Lipo的《Vector Control and Dynamics of AC Drives》第78页的一个例子参数并稍作修改。这个模型没有使用dq坐标系。

本模型中使用的电机主要参数为：

• 额定电压（相电压）：220 V
• 额定频率：50 Hz
• 极对数：2
• 转动惯量：0.1 kg.m^2
• 定子电阻：0.531 Ohm
• 转子电阻：0.408 Ohm
• 定子漏感：2.52 mH
• 转子漏感：2.52 mH
• 互感：8.47 mH

上述参数可根据实际电机的参数进行修改，负载转矩和负载惯量可根据实际仿真情况加以修改。

Modelica模型如下。

model SACIM "A Simple AC Induction Motor Model"
  type Voltage=Real(unit="V");
  type Current=Real(unit="A");
  type Resistance=Real(unit="Ohm");
  type Inductance=Real(unit="H");
  type Speed=Real(unit="r/min");
  type Torque=Real(unit="N.m");
  type Inertia=Real(unit="kg.m^2");
  type Frequency=Real(unit="Hz");
  type Flux=Real(unit="Wb");
  type Angle=Real(unit="rad");
  type AngularVelocity=Real(unit="rad/s");

  constant Real Pi = 3.1415926;     

  Current i_A"A Phase Current of Stator";
  Current i_B"B Phase Current of Stator";
  Current i_C"C Phase Current of Stator";
  Voltage u_A"A Phase Voltage of Stator";
  Voltage u_B"B Phase Voltage of Stator";
  Voltage u_C"C Phase Voltage of Stator";
  Current i_a"A Phase Current of Rotor";
  Current i_b"B Phase Current of Rotor";
  Current i_c"C Phase Current of Rotor";
  Frequency f_s"Frequency of Stator";
  Torque Tm"Torque of the Motor";
  Speed n"Speed of the Motor";

  Flux Psi_A"A Phase Flux-Linkage of Stator";
  Flux Psi_B"B Phase Flux-Linkage of Stator";
  Flux Psi_C"C Phase Flux-Linkage of Stator";
  Flux Psi_a"a Phase Flux-Linkage of Rotor";
  Flux Psi_b"b Phase Flux-Linkage of Rotor";
  Flux Psi_c"c Phase Flux-Linkage of Rotor";

  Angle phi"Electrical Angle of Rotor";
  Angle phi_m"Mechnical Angle of Rotor";
  AngularVelocity w"Angular Velocity of Rotor";

  Torque Tl"Load Torque";  

  parameter Resistance Rs = 0.531"Stator Resistance";
  parameter Resistance Rr = 0.408"Rotor Resistance";
  parameter Inductance Ls = 0.00252"Stator Leakage Inductance";
  parameter Inductance Lr = 0.00252"Rotor Leakage Inductance";
  parameter Inductance Lm = 0.00847"Mutual Inductance";
  parameter Frequency f_N = 50"Rated Frequency of Stator";
  parameter Voltage u_N = 220"Rated Phase Voltage of Stator";
  parameter Real p =2"number of pole pairs";
  parameter Inertia Jm = 0.1"Motor Inertia";
  parameter Inertia Jl = 0.1"Load Inertia";

initial equation 

  Psi_A = 0;
  Psi_B = 0;
  Psi_C = 0;
  Psi_a = 0;
  Psi_b = 0;
  Psi_c = 0;
  phi = 0;
  w = 0;

equation

  u_A = Rs * i_A + 1000 * der(Psi_A);
  u_B = Rs * i_B + 1000 * der(Psi_B);
  u_C = Rs * i_C + 1000 * der(Psi_C);

  0 = Rr * i_a + 1000 * der(Psi_a);
  0 = Rr * i_b + 1000 * der(Psi_b);
  0 = Rr * i_c + 1000 * der(Psi_c);

  Psi_A =   (Lm+Ls)*i_A + (-0.5*Lm)*i_B + (-0.5*Lm)*i_C +        (Lm*cos(phi))*i_a + (Lm*cos(phi+2*Pi/3))*i_b + (Lm*cos(phi-2*Pi/3))*i_c;
  Psi_B = (-0.5*Lm)*i_A +   (Lm+Ls)*i_B + (-0.5*Lm)*i_C + (Lm*cos(phi-2*Pi/3))*i_a +        (Lm*cos(phi))*i_b + (Lm*cos(phi+2*Pi/3))*i_c;
  Psi_C = (-0.5*Lm)*i_A + (-0.5*Lm)*i_B +   (Lm+Ls)*i_C + (Lm*cos(phi+2*Pi/3))*i_a + (Lm*cos(phi-2*Pi/3))*i_b +        (Lm*cos(phi))*i_c;

  Psi_a =        (Lm*cos(phi))*i_A + (Lm*cos(phi-2*Pi/3))*i_B + (Lm*cos(phi+2*Pi/3))*i_C +   (Lm+Lr)*i_a + (-0.5*Lm)*i_b + (-0.5*Lm)*i_c;
  Psi_b = (Lm*cos(phi+2*Pi/3))*i_A +        (Lm*cos(phi))*i_B + (Lm*cos(phi-2*Pi/3))*i_C + (-0.5*Lm)*i_a +   (Lm+Lr)*i_b + (-0.5*Lm)*i_c;
  Psi_c = (Lm*cos(phi-2*Pi/3))*i_A + (Lm*cos(phi+2*Pi/3))*i_B +        (Lm*cos(phi))*i_C + (-0.5*Lm)*i_a + (-0.5*Lm)*i_b +   (Lm+Lr)*i_c;

  Tm =-p*Lm*((i_A*i_a+i_B*i_b+i_C*i_c)*sin(phi)+(i_A*i_b+i_B*i_c+i_C*i_a)*sin(phi+2*Pi/3)+(i_A*i_c+i_B*i_a+i_C*i_b)*sin(phi-2*Pi/3));

  w = 1000 * der(phi_m);

  phi_m = phi/p;
  n= w*60/(2*Pi);

  Tm-Tl = (Jm+Jl) * 1000 * der(w);

  if time <= 100 then
    u_A = 0;
    u_B = 0;
    u_C = 0;
    f_s = 0;
    Tl = 0;
  else
    f_s = f_N;
    u_A = u_N * 1.414 * sin(2*Pi*f_s*time/1000);
    u_B = u_N * 1.414 * sin(2*Pi*f_s*time/1000-2*Pi/3);
    u_C = u_N * 1.414 * sin(2*Pi*f_s*time/1000-4*Pi/3);
    Tl = 10;
  end if;

end SACIM;

在模型中，我们定义了电机的定子电压方程（由于仿真软件的时间单位是毫秒，所以所有求导操作前都乘以1000，下同）：

  u_A = Rs * i_A + 1000 * der(Psi_A);
  u_B = Rs * i_B + 1000 * der(Psi_B);
  u_C = Rs * i_C + 1000 * der(Psi_C);

转子电压方程（针对鼠笼转子，如果采用绕线式转子，可以把外接的电阻和电抗参数引入方程）：

  0 = Rr * i_a + 1000 * der(Psi_a);
  0 = Rr * i_b + 1000 * der(Psi_b);
  0 = Rr * i_c + 1000 * der(Psi_c);

定子磁链方程：

  Psi_A =   (Lm+Ls)*i_A + (-0.5*Lm)*i_B + (-0.5*Lm)*i_C +        (Lm*cos(phi))*i_a + (Lm*cos(phi+2*Pi/3))*i_b + (Lm*cos(phi-2*Pi/3))*i_c;
  Psi_B = (-0.5*Lm)*i_A +   (Lm+Ls)*i_B + (-0.5*Lm)*i_C + (Lm*cos(phi-2*Pi/3))*i_a +        (Lm*cos(phi))*i_b + (Lm*cos(phi+2*Pi/3))*i_c;
  Psi_C = (-0.5*Lm)*i_A + (-0.5*Lm)*i_B +   (Lm+Ls)*i_C + (Lm*cos(phi+2*Pi/3))*i_a + (Lm*cos(phi-2*Pi/3))*i_b +        (Lm*cos(phi))*i_c;

转子磁链方程：

  Psi_a =        (Lm*cos(phi))*i_A + (Lm*cos(phi-2*Pi/3))*i_B + (Lm*cos(phi+2*Pi/3))*i_C +   (Lm+Lr)*i_a + (-0.5*Lm)*i_b + (-0.5*Lm)*i_c;
  Psi_b = (Lm*cos(phi+2*Pi/3))*i_A +        (Lm*cos(phi))*i_B + (Lm*cos(phi-2*Pi/3))*i_C + (-0.5*Lm)*i_a +   (Lm+Lr)*i_b + (-0.5*Lm)*i_c;
  Psi_c = (Lm*cos(phi-2*Pi/3))*i_A + (Lm*cos(phi+2*Pi/3))*i_B +        (Lm*cos(phi))*i_C + (-0.5*Lm)*i_a + (-0.5*Lm)*i_b +   (Lm+Lr)*i_c;

电磁转矩方程：

  Tm =-p*Lm*((i_A*i_a+i_B*i_b+i_C*i_c)*sin(phi)+(i_A*i_b+i_B*i_c+i_C*i_a)*sin(phi+2*Pi/3)+(i_A*i_c+i_B*i_a+i_C*i_b)*sin(phi-2*Pi/3));

转子的角速度和机械角位移存在导数关系：

  w = 1000 * der(phi_m);

下面两个公式实现转子电角度与机械角度，角速度和电机转速之间的单位转换。

  phi_m = phi/p;
  n= w*60/(2*Pi);

电机的实际速度由电机的电磁转矩、负载转矩以及电机和负载的共同负载惯量决定(采用最简化的刚体动力学模型，可逐渐扩展):

  Tm-Tl = (Jm+Jl) * 1000 * der(w);

在此基础上，我们就可以通过设定外部条件的变化来仿真电机的运行，如改变定子电压和频率，定子串电阻，转子串电阻，改变负载大小等。

这里只给出了最简单的额定电压直接启动的例子

  if time <= 100 then
    u_A = 0;
    u_B = 0;
    u_C = 0;
    f_s = 0;
    Tl = 0;
  else
    f_s = f_N;
    u_A = u_N * 1.414 * sin(2*Pi*f_s*time/1000);
    u_B = u_N * 1.414 * sin(2*Pi*f_s*time/1000-2*Pi/3);
    u_C = u_N * 1.414 * sin(2*Pi*f_s*time/1000-4*Pi/3);
    Tl = 10;
  end if;

运行如下命令可进行模型的仿真：

simulate(SACIM,startTime=0,stopTime=2000)